In mathematics, equivariant topology is the study of topological spaces that possess certain symmetries. In studying topological spaces, one often considers continuous maps, and while equivariant topology also considers such maps, there is the additional constraint that each map "respects symmetry" in both its domain and target space. The notion of symmetry is usually captured by considering a Group action of on and and demanding that is equivariant under this action, so that for all, a property usually denoted by . Heuristically speaking, standard topology views two spaces as equivalent "up to deformation," but equivariant topology considers spaces equivalent up to deformation so long as it pays attention to any symmetry possessed by both spaces. A famous theorem of equivariant topology is the Borsuk–Ulam theorem, which asserts that every -equivariant map necessarily vanishes.
Induced -bundles
An important construction used in Equivariant cohomology and other applications includes a naturally occurring group bundle Let us first consider the case where acts freely on. Then, given a -equivariant map, we obtain sections given by, where gets the diagonal action, and the bundle is, with fiber and projection given by. Often, the total space is written More generally, the assignment actually does not map to generally. Since is equivariant, if, then by equivariance, we have that, so in fact will map to the collection of. In this case, one can replace the bundle by a homotopy quotient where acts freely and is bundle homotopic to the induced bundle on by.
In the same way that one can deduce the Ham sandwich theorem from the Borsuk-Ulam Theorem, one can find many applications of equivariant topology to problems of discrete geometry. This is accomplished by using the Configuration-Space Test-Map paradigm: Given a geometric problem, we define the configuration space,, which parametrizes all associated solutions to the problem Additionally, we consider a test space and a map where is a solution to a problem if and only if. Finally, it is usual to consider natural symmetries in a discrete problem by some group that acts on and so that is equivariant under these actions. The problem is solved if we can show the nonexistence of an equivariant map. Obstructions to the existence of such maps are often formulated algebraically from the topological data of and. An archetypal example of such an obstruction can be derived having a vector space and. In this case, a nonvanishing map would also induce a nonvanishing section from the discussion above, so, the top Stiefel–Whitney class would need to vanish.
